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Dye-doped polymer micro-cavity

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Presentation on theme: "Dye-doped polymer micro-cavity"— Presentation transcript:

0 a 3-D investigation of 2-D organic micro-billiard lasers
Light from the edge: a 3-D investigation of 2-D organic micro-billiard lasers Clément Lafargue1, S. Lozenko1 , S. Bittner1, C. Ulysse2, C. Cluzel3, J. Zyss1, M. Lebental1 1 – Laboratoire de Photonique Quantique et Moléculaire, ENS de Cachan. 2 – Laboratoire de Photonique et de Nanostructures , CNRS, Marcoussis. 3 – Laboratoire de mécanique et technologie, ENS de Cachan. 25’’ Joke billiard Molecular quantum photonics lab

1 Dye-doped polymer micro-cavity
Organic microlasers Conventional laser Dye-doped polymer micro-cavity Amplifying medium + Resonating Cavity Usual configuration weak confinement n ≈ 1.5 40’’ Low index = weak confinement, desirable effect Deep reasons : selection of few orbits, WGM: Microsphères et microtores de Silice, Cavity quantum electrodynamics group

2 LPQM – microlaser group topics
Chaotic cavities POSTER, I. Gozhyk : Towards the control of polarization properties of solid state organic lasers I. Gozhyk, PRA 86, (2012) Lebental, APL 88, (2006) Unidirectional lasing N.Djellali, APL 95, (2009) Emission Diffraction Measurement and model POSTER, S. Bittner : Localization of modes in a dielectric square resonator Semi-classical modeling S.Lozenko “Microfluid” EU Project Analyte solution flow Numerical modeling 90’’ Interessé/ intrigué par les directions d’émission , on a s’est retrouvé confronté au problème du coin diélectrique. Mécanisme de sortie -> joue aussi sur la compétition en tre modes vu que pertes=gain De plus on s’est dit qu’on pouvait peut-être apporter qqchose grâce à nos machins sur le prb même du coin diélectrique

3 Motivation: diffraction at dielectric corners and edges
no solution Metallic corner Sommerfeld 1896 30’’ Steady-state Fil rouge diffraction : expliquer les similitudes et différences des différents cas (diff du FP, dif du carré , diff du triangle-diffractiv orbit) A standing wave in a resonator to explore the corner

4 Outline Background on organic microlasers Fabrication Experiment
Emission/diffraction properties Fabry-Pérot like cavities Square cavities Triangular microlasers 20’’ 4

5 Outline Background on organic microlasers Fabrication Experiment
Emission /diffraction properties Fabry-Pérot like cavities Square cavities Triangular microlasers 5’’ 5 5

6 Organic microlaser: Fabrication
Cavity n≈1.5 PMMA + Dye SiO2 n=1.45 n2=1 μm Fabrication: Electron-beam lithography µm Microscope photograph SEM photograph 1μm 0.6 µm µm Arbitrary cavity shapes Different laser dyes 40’’ 6 6

7 Organic microlasers: characterization
Excitation geometry Lasing thresholds pumping 532 nm Emission diagrams ~610 nm emission collecting lens Spectrometer Spectrum L 40’’ Pulsed pumping Typical spectrum Images Wavelength [nm] 7

8 Organic microlasers: characterization
Experimental Measurements Lasing thresholds Emission diagrams Spectrum L 20’’ Images

9 Organic microlasers: characterization
Experimental Measurements Lasing thresholds FAR FIELD DETECTION Emission diagrams Spectrum L 20’’ Dire ‘square’, ‘stadium’ ‘sharp lobes’ Images Physical Review A 75, (2007)

10 Semi-classical approach
Organic microlasers: characterization Experimental Measurements Lasing thresholds F.S.R. Emission diagrams Semi-classical approach Spectrum L 20’’ FSR linked to the length of PO Expliquer differentes PO Images Periodic Orbits PRA 76, (2007)

11 Organic microlasers: characterization
Experimental Measurements Lasing thresholds Emission diagrams Spectrum L 20’’ Images

12 Outline Background on organic microlasers Fabrication Experiment
Emission/diffraction properties Fabry-Pérot like cavities Square cavities Triangular microlasers 10’’ 12 12

13 3D emission- latitude diagrams
FP Measurement: 50’’ Emission UPLIFTED 13

14 3D emission- latitude diagrams
FP Sergey Lozenko J.A.P. 111, (2012) z Measurement: x 50’’ Thin Angular lobes Free-standing 14

15 3D emission - latitude diagrams
FP Model: Slit diffraction Interference (wafer) 50’’ Remind that it is a FP Enlight the differences C. Lafargue, to be submitted 15

16 Outline Background on organic microlasers Fabrication Experiment
Emission/diffraction properties Fabry-Pérot like cavities Square cavities Triangular microlasers 20’’ 16 16

17 Square microlaser : diffractive outcoupling
Diamond orbit confined by total internal reflection … nL = n x 2√2 a 50’’

18 Square microlaser : diffractive outcoupling
Diamond orbit confined by total internal reflection … … but losses occur via diffraction 30’’ 18

19 Square microlaser : diffractive outcoupling
Pump : 30’’ + example pola effect Camera Pump polarization effects I. Gozhyk, PRA 86, (2012),

20 Square microlaser : diffractive outcoupling
The diffraction at the corners here is not at all understood, but it would be important to do so the latitude diagrams depend strongly on the kind of mode inside the resonator -> maybe there is some kind of connection between the diffraction in the two different directions.

21 Outline Background on organic microlasers Fabrication Experiment
Emission/diffraction properties Fabry-Pérot like cavities Square cavities Triangular microlasers 20’’ 21 21

22 Periodic Orbits in triangles
A not so simple shape (not regular contour) No totally confined periodic orbits An open mathematical question:  «  Does a periodic orbit in a triangle exist ? » Alain Grigis, University Paris XIII ?

23 FP winning 100° 40°

24 FP not always winning Camera view 110° 35° 35° 110°
Despite the fact FP is in family, the other isolated orbit is winning

25 Diffractive orbit 98.04° 40° 41.96° « DO not exist in classical mechanics »

26 Summary Diffraction effects from the edges on different contours :
3D Fabry-Pérot emission well understood Square : emission at the corners 3D emission depends on the cavity shape Triangles Identification of orbits Switching between different types of orbits Observation of a diffractive orbit

27 Perspectives 5’’

28

29 110° 110° 700

30 phi= 60° phi= -22° Incidence 0° Incidence 40°

31 Does a periodic orbit in a triangle exist ?
Alain Grigis, University Paris XIII Acute triangles feet of the altitudes Less than 100° triangles: Journal of Experimental Mathematics, 18, p. 137 (2008) Rational triangles : angles = pp/m , unfolding theory Others … 31

32 Information in the laser spectrum : Length L of the periodic orbit
Semi-Classical point of view Information in the laser spectrum : Length L of the periodic orbit Lasing L n1 n2 32 32

33 Periodic orbits & trace formula
Density of states Wave physics Semi-classical limit Classical physics PRE 83, (2011) Sum on periodic orbits Length of the orbits Fresnel reflexion coefficients Coeff depending only on classical quantities

34 Effective index approximation
Electromagnetism z Passive cavity (no laser) : resonances w ? Boundary conditions Outside Inside (Dxy + neff ² k²) z Effective index approximation 34

35 From electromagnetism to wave chaos
2D problem Boundary conditions diffraction 35

36 Resonance computation
Square: not integrable Diamond -1.2 100 Charles Schmit, Eugène Bogomolny Phys. Rev. E 83, (2011) 36

37 How to fabricate ? What are the emission directions ?

38 3D – Polarization selection
q q Pump polarization Camera 38

39 3D – Polarization selection
Pump polarization : (Camera) 39


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